{"arxiv_id":"hep-ph/0306001","incoming":{"papers":8,"sentences":9,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":6,"sentences":6,"quotes":[{"arxiv_id":"0704.1800","title":"Phenomenology with Massive Neutrinos","url":"/paper/0704.1800","section":"Global $3ν$ Analysis of Oscillation Data","sentence":"As described in Ref. [ref] the leptonic mixing matrix can be consistently extracted as follows.","intent_p":0.94,"contests_p":null},{"arxiv_id":"2010.00440","title":"Leptonic CP Violation and its Origin","url":"/paper/2010.00440","section":"Results: leptonic mixing matrix and CP violation","sentence":"From the global $χ^2$ analysis described in the previous section and following the procedure outlined in Ref. [ref] one can derive the $3σ$ ranges on the magnitude of the elements of the leptonic mixing matrix:","intent_p":0.93,"contests_p":null},{"arxiv_id":"1611.01514","title":"Updated fit to three neutrino mixing: exploring the accelerator-reactor complementarity","url":"/paper/1611.01514","section":"Results: leptonic mixing matrix and CP violation","sentence":"From the global $χ^2$ analysis described in the previous section and following the procedure outlined in Ref. [ref] one can derive the $3σ$ ranges on the magnitude of the elements of the leptonic mixing matrix:","intent_p":0.94,"contests_p":null},{"arxiv_id":"2410.05380","title":"NuFit-6.0: Updated global analysis of three-flavor neutrino oscillations","url":"/paper/2410.05380","section":"Global analysis","sentence":"Altogether, we derive the following $3σ$ ranges on the magnitude of the elements of the leptonic mixing matrix (see Ref. [ref] for details on how we derive the ranges and their correlations):","intent_p":0.93,"contests_p":null},{"arxiv_id":"1811.05487","title":"Global analysis of three-flavour neutrino oscillations: synergies and tensions in the determination of theta_23, delta_CP, and the mass ordering","url":"/paper/1811.05487","section":"Summary of global fit results","sentence":"Note that there are strong correlations between the elements due to the unitary constraint, see Ref. [ref] for details on how we derive the ranges.","intent_p":0.8,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0803.2039","title":"Lepton flavour violating semileptonic tau decays in constrained MSSM-seesaw scenarios","url":"/paper/0803.2039","section":"LFV in the SUSY-seesaw scenario","sentence":"Concerning our choice for the size of the physical neutrino parameters, we shall focus in this work on scenarios where both light and heavy neutrinos are hierarchical, [equation] and set the numerical values for the light neutrino parameters to the following ones which are compatible with present data [ref] [equation] Notice that, for simplicity, the three CP violating phases, have been set to zero.","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":2},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[{"relation":"same_result","label":"States the same result","papers":[{"arxiv_id":"hep-ph/0410030","url":"/paper/hep-ph/0410030","title":"Global Analysis of Neutrino Data","main_claim":"I derive the allowed ranges for the mass and mixing parameters when the bulk of data is consistently analyzed in the framework of mixing between the three active neutrinos and obtain as a result the most up-to-date determination of the leptonic mixing matrix.","p":0.96}]}],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/0306001"}}